|Publication number||US7820977 B2|
|Application number||US 11/690,150|
|Publication date||Oct 26, 2010|
|Priority date||Feb 4, 2005|
|Also published as||US20070187608|
|Publication number||11690150, 690150, US 7820977 B2, US 7820977B2, US-B2-7820977, US7820977 B2, US7820977B2|
|Inventors||Steve Beer, Dan Inbar|
|Original Assignee||Steve Beer, Dan Inbar|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (210), Non-Patent Citations (15), Referenced by (5), Classifications (6), Legal Events (1)|
|External Links: USPTO, USPTO Assignment, Espacenet|
The present application is a continuation in part of U.S. patent application Ser. No. 11/463,112 filed Aug. 8, 2006 (published Dec. 28, 2006 as US Patent Publication 2006/0289775) and claims the benefit under 35 U.S.C. §1.19(e) of U.S. Provisional application 60/767,379 filed Mar. 23, 2006, 60/891,551 filed Feb. 26, 2007, 60/891,727 filed Feb. 27, 2007, 60/891,729 filed Feb. 27, 2007, 60/891,738 filed Feb. 27, 2007, 60/891,751 filled Feb. 27, 2007, 60/892,254 filled Mar. 1, 2007 and 60/892,893 filled Mar. 5, 2007. U.S. patent application Ser. No. 11/463,112 is a continuation in part of U.S. patent application Ser. No. 11/348,040 filed Feb. 6, 2006 (published Dec. 28, 2006 as US Patent Publication 2006/0284094), which claims the benefit under 35 U.S.C. §1.19(e) of U.S. Provisional Applications 60/649,541 filed Feb. 4, 2005; 60/651,622 filed Feb. 11, 2005; 60/654,964 filed Feb. 23, 2005. This application also claims the benefit under 35 U.S.C. §1.19(e) of U.S. Provisional Applications 60/706,013 filed Aug. 8, 2005; 60/706,752 filed Aug. 10, 2005; 60/707,154 filed Aug. 11, 2005; 60/709,428 filed Aug. 19, 2005; 60/710,891 filed Aug. 25, 2005; 60/596,769 filed Oct. 20, 2005; 60/596,814 filed Oct. 24, 2005; 60/597,354 filed Nov. 28, 2005; 60/597,434 filed Dec. 1, 2005; 60/597,435 filed Dec. 1, 2005, 60/597,569 filed Dec. 10, 2005; 60/597,629 filed Dec. 14, 2005.
All of the above mentioned applications and publications are incorporated herein by reference. Patent publications 2006/0289775 and 2006/0284094 are referred to herein as “the above referenced publications.”
The present invention is in the field of threat detection.
For a number of years governments have been struggling with how to keep terrorists from trafficking in special nuclear materials (SNM) and devices containing such materials and radiological dispersion devices (RDD). Such materials include weapon grade Uranium (WGU) and weapon grade Plutonium (WGP) and radioactive sources used for RDD. Such trafficking can take place by people, car, truck, container, rail, ship or other supply chain means. There is a long perceived need for a cost/effective system to screen, detect, locate and identify SNM or RDD materials or devices that are being transported. Furthermore there is a long felt need for an effective means to scan, locate and identify suspected areas in which those threats may be present.
Such screening is difficult in practice due, at least in part, to the environment in which it is done. Firstly, environmental radiation (including terrestrial and atmospheric radiation) of gamma rays and neutrons is substantial. Secondly, benign Normally Occurring Radiological Materials [NORM] like K-40 occur in nature and are present in many benign cargos. For example, kitty litter, plywood, concrete and bananas, emit substantial amounts of benign radiation. Additionally, humans undergoing nuclear medicine imaging or radiation treatment using implanted radioactive seeds can emit sizeable amounts of radiation. These and other “natural” or “benign” sources of radiation coupled with the ability to shield (using high Z materials like lead to shield gammas and some low Z materials to shield neutrons) the SNM and RDD, make simple detection schemes either ineffective in finding nuclear radiological threats or prone to a poor receiver operating characteristic (ROC), for example by having a large percentage of false positives.
Substantial numbers of false positives (also called ‘false alarms’) produce a large number of screened objects (e.g. vehicles, people, cargo) that have to be searched or otherwise vetted manually, making such simple systems practically useless for screening large numbers of objects. At present the leading means to screen RDD and SNM trafficking vehicles are the so called next generation Advanced Spectroscopic Portals (ASP) developed recently for the U.S. DHS DNDO.
More than 90% of the ASP systems use an array of 8 or 16 relatively small NaI(Tl) scintillators (e.g., 0.1×0.1×0.4 meter), to detect the gamma energy spectroscopic signatures of SNM and RDD, and a small array of He-3 Neutron detectors to detect and count neutron emissions.
ASP systems do not provide nuclear imaging, of either gamma rays or neutrons. ASP systems detection performance is limited primarily due to the high cost of NaI detectors, which limits the system detection area/sensitivity. Because of the high price and practical cost constraints of the NaI(Tl) and He-3 detectors, their number is small [typically the ASP NaI detectors have a sensitive area of 0.64 meter2] relative to the distance from the threat radiation source, resulting in a small solid angle of the detector as viewed by the threat. This limits the detection sensitivity and selectivity.
It is noted that while, for a given stand-off distance, the total detected radiation (benign radiation and the threat radiation) is proportional to the solid angle subtended by the detectors at the emitting radiation sources, the background radiation sigma (statistical standard deviation) is proportional to the square root of the solid angle. Thus, a 100 fold increase in solid angle (≈detector size) results in a 10 fold increase in detection certainty (number of standard deviations above the signal mean) to threats in a given screening condition. For example, if the small area (i.e. small solid angle) could reliably detect a source with 10 micro Curie of activity, the 100 times larger detector will detect 1 micro Curie with the same certainty (same rate of true and false detections, given the same geometry and background radiation).
Furthermore, the ASP detects only one threat signature for WGU and RDD—its gamma spectroscopic signature, since such materials do not emit neutrons in an amount much different from background. For WGP it detects also as a second signature its neutron emission. Having only one or two signature detection capabilities makes the system less reliable.
In addition, ASP systems do not provide several other SNM-RDD signatures such as 1D, 2D and 3D nuclear imaging, temporally based signatures such as cascade isotopes (e.g. Co60) doublets detection and gamma/neutron salvo emanating from spontaneous fission of SNM. Having such additional signatures would improve the ROC.
These and other limitations are known in the art and drove the DHS DNDO to publish the BAA-06-01 document. This publication states the need to come up with transformational technologies which will provide a much better than ASP SNM signatures detection performance, such as lower cost detectors, improved energy resolution detectors, the use of other than gamma energy spectroscopy SNM-signatures (e.g. spontaneous fission signature, imaging), detection of incident gamma or neutron directionality and other means that improve the overall system ROC.
The prior art teaches that organic scintillators (OS) provide a highly robust and stable material that is easily formable in many shapes, with the best detection sensitivity when cost per detected Gamma events is considered. On the other hand, there is a common belief in the prior art that organic scintillators, although some non-spectroscopic OS based portals have been used in the past, fail to provide acceptable ROC as they do not provide energy resolution (or at best a very limited one) in the context of nuclear threat detection. This explains why organic scintillators haven not been used for direct gamma spectroscopy isotope identification in nuclear radiological spectroscopic portals (NRSPs) (in the way NaI(Tl) and HPGe detectors are used in ASP) to identify and/or provide reliable energy window of SNM, RDD and NORM selected gamma energies. Furthermore, it is accepted that for all practical purposes screening portals organic scintillators have a poor gamma efficiency or “stopping power” at energies above 300 keV as compared to NaI(Tl). A review of this issue is given in: Stromswold, D.C. et al., “Comparison of plastic and NaI(Tl) scintillators for vehicle portal monitor applications” in: Nuclear Science Symposium Conference Record, 2003 IEEE, Vol (2) pp. 1065-1069. October 2003. The disclosure of this paper is incorporated herein by reference.
In recent studies related to anti-neutrino detection (see http.//arxiv.org/ftp/physics/papers/404/0404071.pdf) and in other publication of the same group (see F. Suekane et al., “An overview of the KamLAND 1; K-RCNP International School and mini-Workshop for Scintillating Crystals and their Applications in Particle and Nuclear Physics Nov., 17-18, 2003, KEK, Japan, it has been shown that extremely large (8 meter diameter) expensive (>$100 million, due mainly to the very large detector size and large number of large [18”] photomultiplier tubes (PMTs) used) liquid scintillator detectors can provide gamma energy resolution which is close to that of NaI(Tl). Such devices are not practical for large scale (or even small scale) deployment for threat detection due to their geometry and astronomical cost. The disclosure of this paper is incorporated herein by reference.
R. C. Byrd et al., in “Nuclear Detection to Prevent or Defeat Clandestine Nuclear Attack”, IEEE Sensors Journal, Vol. 5 No. 4, pp. 593-609, 2005, present a review of prior art of SNMRDD screening, detection and identification techniques. The disclosure of these papers is incorporated herein by reference.
In a PNNL report by Reeder, Paul L. et al., “Progress Report for the Advanced Large-Area Plastic Scintillator (ALPS) Project: FY 2003 Final” PNNL-14490, 2003, a PVT light collection efficiency of 40% for a 127 cm long detector is described. It should be noted that a straight forward extension to 4 meters length of the PNNL OS approach would have resulted in less than 25% light collection and less than 15% light collection for a 6 m long detector. The disclosure of the PNNL report is incorporated herein by reference.
The above referenced patent publications describe a number of embodiments that ameliorate some or all of these problems. For example, these publications describe a number of structures to detect radiation particles, such as those emitted by nuclear threats with increased efficiency and spectral purity. Some embodiments utilize thick plastic or liquid scintillator materials to increase the capture efficiency and allow for more accurate determination of the captured radiation particles. In general the energy in the particles is captured in a number of interactions, in which the radiation gives up energy converted into light scintillations. As mentioned therein, despite the thickness of the detector, for some particles, a portion of the energy is not captured due to what are described as “escape quanta”, namely uncaptured secondary radiation which escapes from the detector. U.S. 2006/0289775 mentions in paragraph  that it is possible to discriminate particles that do not give up all their energy based on the number of interactions that take place and result in scintillations.
Further information on the state of the art can be found in the Background section of and referenced prior art listed and included by reference in the above referenced U.S. patent application and provisional patent applications.
As indicated US Patent publications 2006/0289775 and 2006/0284094 “the above referenced publications” are incorporated herein by reference and the present application is a continuation in part thereof. Thus the inclusion of them in the background section should not be considered to be an admission that the claims hereof are anticipated by 35 U.S.C. §102. It is noted that the invention claimed herein was not claimed in the earlier applications and that this invention is a joint invention of the inventors of the present application.
The above referenced publications are very long and describe detectors for nuclear radiation and systems and methods which utilize these detectors. Since the present invention is mainly concerned with methods of improving them, the description of systems that utilize the detectors is not described herein in detail. Rather, applicants rely on the incorporation by reference of the above referenced application for support of any claims utilizing the improvements described herein.
An aspect of some embodiments of the invention is concerned with methods for the improvement in the spectral sensitivity of detectors in which “escape quanta” cause a reduction in the spectral sensitivity. It is especially useful in conjunction with detectors of a type described in the above referenced publications.
In some embodiments of the invention, incoming radiation particles/photons for which some of the energy escapes without causing scintillations in the detector are identified based on the number of scintillations that the particle creates as it interacts with the detector material and loses its energy. In some embodiments of the invention, the incident energy identification is based on one or more metrics or scores, such as the time between the start of the first and last recorded scintillations, the distance from a surface of the detector of the last detected scintillation, the number of separate scintillator elements in the detector that produce scintillations from the event and/or the number of scintillation events, as well as the overall volume or size of the ‘scintillation envelope’.
In an exemplary embodiment of the invention, the detector is segmented such that gamma rays can be transmitted substantially without impediment between segments while light generated by scintillations within a segment stays substantially within that segment and is individually measured.
Optionally, the detector is a planar detector formed as a series of elongate detector segments placed side by side. Preferably, the detector is also segmented in a direction normal to the plane of the detector, by light reflecting, low radiation attenuating barriers, such that light from scintillations that occur at different depths in the detector are confined to the detector segments in which they occur. Since the barriers are substantially transparent to gamma and neutron radiation, gamma and neutron radiation that contains residual energy after a given scintillation can pass substantially unimpeded to a different segment. For nuclear threat detection in objects, such as trucks and maritime containers a 4 m×4 m×0.5 m detector assembly is typically segmented into 200 elongated segments, each measuring 0.1 m×0.1 m×4 m. However, the cross-section of the elongate segments can have various other forms in addition to the rectangular form indicated above.
In an exemplary embodiment of the invention, at least two photo-sensors, such as a photomultiplier tube (PMT), are optically coupled to the ends of each segment. The coupled photo-sensors collect light from the ends of the scintillator segments.
By comparing the time and/or intensity of the scintillation light detected at the two photo-sensors (or signals generated by the photo-sensors in response to the light), the position of the initial scintillation within of the segment can be estimated using one or both of time of flight (TOF) techniques and the ratio of the PMT signals. As the total charge emanating from the two PMTs is integrated, it represents the total collected light, which can be used to determine the deposited energy of the scintillation, especially after the segment is calibrated as described herein.
Thus, a two dimensional array of such elongate segment can be used to localize the position of the incident particle scintillation within the detector assembly in three dimensions. By summing the signals produced by the individual PMTs in response to the scintillations, determine the incident particle energy, assuming full energy deposition within the detector volume.
It should be understood that such scintillators can be made of any scintillating material. However, the present inventor has found that organic scintillators and especially liquid organic scintillators (LS) have the requisite requirements for detection of nuclear threats. Typical LS for use in the invention comprises a cocktail of (for a 4 m×4 m×0.5 m volume detector) 12 kg PPO, 6.3 m3 normal-dodecane and 1.6 m3 pseudo cumene. The barriers can be of many materials. Some useful materials are thin nylon sheets, coated with a thin layer of reflecting paint, or sheets of naturally reflective Teflon. In some embodiments of the invention, the segments are formed by creating such partitions in a vessel filled with LS material.
In an embodiment of the invention, the detector is a 2D imaging detector. It is capable of imaging suspected one or both of gamma rays and neutrons. In one embodiment, the detector is fitted with high Z (e.g. lead) collimators for gamma collimation. Alternatively or additionally, the detector is formed of segments, some of which act as collimators for other segments, since they absorb both gammas and neutrons. This second option is also useful for imaging neutrons.
Alternatively or additionally, gross direction capability for both incident gammas and neutrons is achieved even without collimators. As to gamma rays, the incident gamma rays produce a number of scintillations as they travel through the detector segments. The side of the detector, the 2D positions facing the screened item, sub-nanosecond event times, and deposited energy of these scintillations are determined, and a gross direction of incidence of the gamma ray is estimated from analysis of positions of the first and second scintillations emanating from the incident particle interaction with individual segments. This methodology is especially useful in reducing terrestrial and atmospheric radiation by a veto on particles that most probably come from a direction other than the direction of the screened object. As to neutrons, it is possible to determine if the neutrons entered the detector from the top, sides, front side facing the screened object or rear side facing to screened object, since neutrons of typical WGP spontaneous fission energies are captured within the first 5-10 cm of OS detector material. This enables the rejection of more than a half the environmental neutron radiation and an increase in selectivity (e.g., improved ROC) of the system.
Optionally, since a number of images are obtainable as the vehicle passes the large detector, linear (partial views) tomography using one or two slanted collimation means or trans-axial tomography can be performed by using more than two detectors. There is also a possibility to provide concurrently linear and transaxial tomography. Techniques for performing such tomography in the field of X-ray and nuclear tomography are well known, but have not been applied to nuclear threat detection.
An aspect of some embodiments of the invention is concerned with large area detectors (optionally imaging detectors) preferably having >75% stopping power at 0.1-3 MeV gamma energy range suitable for screening a threat vehicle or object, such as a person, car, truck, container, package, train, aircraft or boat. Generally speaking, such detectors are very expensive due to the cost of the detector assembly, the costs of scintillators and/or the costs of the relatively large numbers of photo-sensors or direct nuclear detectors like high purity germanium HPGe detectors that are required. A segmented OS (e.g. LS or Plastic Scintillator) detector according to some embodiments of the invention allows for the construction of a large detectors having extremely high sensitivity for both neutrons and gammas, NaI(Tl) like gamma energy resolution, temporal resolution and intrinsic gamma and neutron spatial resolution that are suitable for reliable nuclear/radiological threat detection for the cost of the most advanced prior art methods.
In some embodiments of the invention a loci dependent light collection efficiency correction is applied to the detector segments energy signals. This correction mitigates a significant variable of loci dependent scintillation light collection efficiency, resulting in a better energy resolution.
In a preferred embodiment of the invention, a segmented LS detector having high light reflecting partitions, coupled to PMTs photocathodes which cover more than 73% of the segments cross section is used. In some embodiments, LS filled optical couplers are used to match the sizes of the PMT and the segments. Such segments use OS such as the PPO based LS described above which have a “mean attenuation length” larger than 15 meters, an index of refraction of approximately 1.5 to match the PMT glass index of refraction, while the PPO emission spectrum matches the sensitivity spectrum of Bi-alkali PMTs. The PMT face is preferably in contact with the LS.
This ensemble may, under some circumstances, provide near 50% light collection efficiency, even for long 3-6 meter detector segments. This increases the number of photoelectrons per MeV at the PMTs, resulting in better energy resolution timestamp and neutron/gamma ID precision. It should be noted that one of the reasons that caused the prior art to believe that OS detectors had poor gamma spectroscopic ability was the low light collection efficiency of elongated scintillators that might be useful for threat detection.
In some embodiments of the invention an OS scintillator assembly larger than 1×1×0.4 meter is used to allow most of the incident gammas having energies of 2.6 MeV or more to substantially deposit their full energy in the scintillator assembly, thus eliminating much of the gamma energy resolution loss due to escape quanta associated with smaller detectors.
In a typical embodiment, a scintillation detector approximately 50 cm deep can have a 4×4 or 6×4 (length×height) meter front face. Larger devices can be constructed, and smaller sizes, such as 2×2 m can be useful for “car size only” or pallets lanes. Such large detectors have a number of potential advantages. One advantage is that the efficiency of capture of both gammas and neutrons emanating from the screened field of view is greatly improved, due to the large subtended angle that they present to the radiation sources. If radionuclide imaging using high Z collimators is implemented this high gamma sensitivity hike is reduced. A second advantage is that the efficiency of detecting temporally coincident SNM RDD signatures like cascaded isotopes and spontaneous fission gamma/neutron salvos is increased. For example, doublet capture is greatly improved, since the probability of doublet capture is roughly the square of the probability of singlet capture. A substantial percentage of doublet capture results in improved discrimination between some doublet emitting threats like Co−60 (used in some RDD designs) and benign radiation and improved sensitivity to threatening radiation. It should be noted that the probability of random chance detectability of doublets is extremely low as the background radiation rate is low approximately 1-3 kcounts per second per square meter, while the doublets detection temporal coincidence window is short (about 20 nanosec).
Another advantage of large detectors, especially imaging detectors, is the amount of time each portion of a moving vehicle is screened. Taking into account the movement of the vehicle, every portion of the moving vehicle stays within range longer and provides a better detected signal.
Some embodiments of the detectors can identify the general or gross direction of an incident gamma and/or neutron particle independent of the use of a collimator and/or shielding. In an embodiment of the invention, at least some events that are incident from a direction other than a direction from which they are expected when screening an object, can be rejected. This allows for a decrease in background radiation both from environmental radiation and from radiation emanating from other objects (e.g. nuclear medicine patients outside the field of screening). In addition, it enables the rejection of events that enter from the back, sides, top and bottom of the detector. Rejecting events that do not come from the expected direction can increase the reliable threat detectability of the system many fold.
Some systems utilizing the detectors provide one or a plurality of energy windowed images on an isotope-by-isotope basis. This technique is used in nuclear medicine imaging applications to provide maps of individual isotopes. Providing maps for different isotopes in threat detectors improves the image and its point source contrast over the background radiation. The efficacy of such windowing is improved by the methods of the present invention.
Organic scintillator with which the present invention may be used may have both intrinsic spatial and temporal resolution and spectrographic properties to discriminate between isotopes. In an embodiment of the invention, the presence of escape quanta can be detected for a given incident particle, and the event vetoed. This can provide a significant improvement in spectroscopic isotope identification.
The combination of high light detection efficiency and high and uniform collection efficiency associated with loci dependent light collection variation correction and the small rate of escape quanta (due to the large detector) allows for gamma spectroscopic isotope I.D. that is similar to that of detectors with NaI(Tl) scintillators. It should be noted that the exact design of the detector is dependent on a tradeoff between gamma spectroscopic identification and imaging capability. If imaging capability is desired, then some kind of collimation may be required. This reduces the capture efficiency based threat signatures performance. On the other hand, if high particle collection efficiency is desired, for spectroscopy, and temporal coincidence signatures (e.g. cascading isotopes I.D. spontaneous fission gamma/neutron I.D.) detection (discussed below) having no collimators may be preferable, to maximize overall sensitivity. In some embodiments, a combination of areas that have collimation and areas that do not have collimation provide a compromise design. Such embodiments are discussed herein.
It is noted that gamma rays give up their energy inside an organic scintillator material in a series of time and geometrically spaced events (e.g. Compton interactions), each of which produces a separate scintillation. In general, it is preferred to have the size of the segments matched to a mean length between scintillations (this indicates a compromise between low [100 keV gammas having a short distance] and high energy gammas [2.6 MeV having a long distance]), such that the position of each event in the detector is, with high probability, in a different segment. The time constant of a single scintillation is the same order of magnitude (a few nanosec) as the time between scintillations of the same event, hence they can not easily be discriminated from each other by time if they occur inside one measurement channel. If, however, they occur in different segments, their leading edge timestamp, deposited energy and 2D location are separately detected and measured. This allows the use of algorithms used in Compton imaging techniques to detect the gross directionality of the incident gamma, and also allows rejection of gammas that are incident from the back face and to a great extent terrestrial and atmospheric gammas and neutrons.
There is thus provided, in accordance with an embodiment of the invention, a method of improving energy determination of a Gamma event which interacts with a segmented scintillation detector, the method comprising:
identifying radiation events detected by a detector that are likely not to have deposited their full energy in the detector, based only on characteristics of said detected events; and
treating the identified radiation events differently from other radiation events that are likely to have deposited their full energy in the detector.
In an embodiment of the invention, identifying comprises determining the number of scintillations caused by a radiation event. Optionally, treating the identified events differently comprises rejecting radiation events causing a number of scintillations below a threshold number.
In an embodiment of the invention, treating the identified events differently comprises rejecting radiation events causing a number of scintillations below a threshold number.
In an embodiment of the invention, identifying events comprises estimating a position and time of scintillations caused by said interactions.
In an embodiment of the invention, identifying is responsive to one or more characteristics chosen from the group consisting of (a) the number of scintillations associated with a given radiation event; (b) the distance of a final scintillation associated with a given radiation event from a boundary of the detector; (c) the time duration of a series of scintillations resulting from a radiation event; or (d) the number of scintillations resulting from a given radiation event. Optionally, the event is rejected is the number of scintillations is below a given number. Optionally, identifying is responsive to at least one, two or to all of (a) (b) or (c).
Optionally, identifying is responsive to at least two three, or all of (a) (b), (c) or (d).
In an embodiment of the invention identifying comprises weighting a probability factor associated with each of said characteristics to provide a score. Optionally, treating differently comprises rejecting events having a weighted score below a given threshold. Optionally, treating differently comprising estimating the energy of said events and utilizing said events with the estimated energy to form an energy spectrum.
In an embodiment of the invention, the scintillator is an organic scintillator.
Exemplary, non-limiting, embodiments of the invention are described below in conjunction with the following drawings, in which like numbers are used in different drawings to indicate the same or similar elements.
As shown in the exemplary embodiment of
Organic scintillators have various advantages over other scintillators, including robustness, stability and low cost, ease of manufacturing and forming, etc. Its two major deficiencies relative to the commonly used NaI(Tl) scintillator are lower stopping power and lower scintillation efficiency of about 10,000 Photons/MeV. Both of these deficiencies are compensated for in some embodiments of the invention.
Organic scintillator materials are well known and have been used for simple detectors which are not used for gamma spectroscopic applications nor for imaging applications.
While the rectangular segments can be either self supported or partitions within a liquid vessel, it is believed that cylindrical segments have to be self supported.
Alternatively or additionally, the rectangular segments are spaced from each other.
If solid OS segments are used, then the construction is simpler and all that is needed is to form the segments and paint them with light reflecting paint, or otherwise provide for good reflectivity.
When a scintillation takes place, the light generated is emitted in all directions. Thus, some of the light travels toward one end and is detected by one of the PMTs and some travels in the other direction and is detected up by the other PMT. Any light photons that are not directly aimed along the elongated segment, will reflect off the reflective walls, possibly multiple times and arrive at the end with a slight delay compared to the directly aimed photons. Since the velocity of light in the scintillation medium is known, the time difference between the ‘leading edge’ of the light signal by the two PMTs is indicative of the position of the interaction along the length of the segment. This method is known in the art as Time of Flight (TOF) localization. In addition since there is some path length dependent attenuation of the light as it travels through the scintillator material, the amplitude of the light is different at the two ends if the scintillation does not occur at the exact midpoint. In an embodiment of the invention one or both of the TOF and amplitude ratio are used to determine the position of the scintillation along elongate segment 204.
Since both time differences and amplitude ratio are affected by other factors, the segments are preferably calibrated using a procedure described below.
As was shown in the incorporated US Patent publication 2006/0284094, with respect to FIGS. 27-29, elongate detectors can be used as threat detectors with one dimensional position discrimination. As can be seen from
Scintillation materials of the preferred type detect both neutrons and gamma rays. However, the footprints of scintillations that are produced are different. In both cases, the energy of the incoming radiation is given up via a series of interactions, which result in scintillations. However, the distance between such events is different, being substantially longer for the gamma rays than for neutrons of typical threat detection energies. In an embodiment of the invention, the depth and height of the segments is such that, in many cases, a single scintillation takes place in a particular segment for gamma rays, while multiple interactions, possibly most of the elastic collision interactions, may take place in one or two detector segments for neutrons of energies that are expected from fissile materials.
Another difference is the scintillation rate of decay for the two types of interactions, especially when all the scintillations caused by an incoming event are considered. This phenomenon is well known and has been used to discriminate between gamma rays and neutrons in non-imaging detectors using PSD methods.
In threat detectors the rate of incoming events is generally low at rates of a few thousand counts per second per meter2. At such low rates, the probability that two scintillations from different incident gamma events will take place in a nearby location at the same time window is low; hence each incident particle and its associated scintillations can be analyzed individually. If the signals produced by the PMTs are time stamped and digitized, then scintillations in different segments can be correlated and scintillations caused by a single incident particle can be grouped and analyzed collectively. The utility of this information will be described below.
In the preferred embodiment of the invention, the partitions are substantially transparent to gamma rays and other quanta such as higher energy electrons, neutrons and protons. Thus, while light is trapped within a particular segment, residual energy, in the form of a gamma ray, or other quanta, not converted to light (or heat) in a particular interaction can pass through the partition into a neighboring (or farther) segment.
In an exemplary embodiment detector 200 comprises a plurality of layers of segments, arranged in the direction perpendicular to front face 202, as shown in
As shown in
A statistical most probable incoming direction of the event can be calculated. This direction is only a gross direction and is generally not sufficiently good for imaging. However, it does enable substantial rejection of background radiation such as terrestrial and atmospheric radiation. This is based on the fact that the direction of the gamma particle having the residual energy after Compton an interaction is related to the incoming direction. Generally, the most probably incoming direction is a straight line between the first and second scintillations.
It should be noted that since detector 200 collects light from all of the scintillations caused by the incident gamma rays, the light collected by scintillator 204 can be used for spectroscopic isotope identification. The spectral resolution depends on a number of factors, some of which are correctable. One of these is a systematic variation in light collection efficiency as a function of position or locus of the scintillation within a segment. In general, the main variable in this respect is the distance and average number of reflections that light from a scintillation event has to undergo in order to reach each of the photomultiplier tubes. This is a constant geometric factor which can be calculated (or measured for a typical segment, as described below) and an appropriate correction made to the energy signal (integral of the light received) indicated at the front-end electronics or system software, based on the determined scintillation position along the segment.
Other correctable variations are gain and delay variations among the individual PMTs. These can also be determined as part of an overall calibration for the segment.
In an experimental calibration of loci dependent light collection efficiency variation correction, according to an embodiment of the invention, a point source of mono-energetic gamma rays or high energy mono-energetic betas is placed adjacent to an individual segment and the energy signals provided by the sum of the two PMTs is measured. This is repeated for a number of positions along the length of the segment. Interactions between the OS material in the segment and the ray will cause scintillations. The signals generated by these scintillations in the PMTs at the end of the segments can be used to define a ratio of signals and a time delay between signals as a function of actual position along the segment.
For betas, the entire energy is transferred in a single interaction. However, for gamma, the energy transferred in the interactions (and the energy in the scintillations) is variable. However, the peak energy scintillations can be assumed to be the result of a direct photoelectric effect interaction (or otherwise a full energy deposition within the segment) and thus their energy is known (i.e., it is the energy of the incoming gamma). This known energy and position can be used as a standard for generating a position dependent energy correction table.
This measurement is repeated for all of the segments and used to provide a look-up table of corrections which enable the conversion of pairs of time-stamped light signals into energy signals and position values, which are used in the method described with respect to FIG. 12 of US Publication 2006/0289775.
Alternatively, the energy collection efficiency can be assumed to be the same for all the segments. Similarly, the collection efficiency as a function of position along the segment can also be assumed to be the same for all segments. Thus, measurements of energy signal correction factors can be approximated for all of the segments, by measurements on a single segment. Such approximation can be expected to give poorer spectral results than when energy correction is based on individual measurements of each detector.
Alternatively, the absolute energy sensitivity of the individual segments is measured, and the spatial distribution is assumed to be the same for all segments. In order to do this, an energy measurement, as described above is performed, but only for a single point along the length of the segment. The sum of the values of the signals is compared to a standard and the energy efficiency of collection is determined by the ratio of the signals. Optionally, the standard is based on measurements of a number of segments. It is noted that this alternative also gives a time difference between the detectors on both ends of the segment.
However, neither this nor the other alternative methods of energy signal calibration allow for determination of an absolute time delay, which is used for some embodiments of the invention.
Absolute time delay (and a correction for such delay variations) for each PMT channel can be determined by feeding a light signal that simulates a scintillation into the segment and then measuring the time delays of the signal outputs by each of the two PMTs at the ends of the segment. If the signal is fed into center of the segment for all of the segments, the time delays of all of the PMTs channels for all the segments can be determined so that a comparison of the times of the signals from each PMT can be used to provide a consistent time stamp for each scintillation event.
It is noted that the segments partitions are coated by a light reflecting material, or a reflective Teflon sheet is used. In order to feed light into the segment, a very small portion of the segment is left uncoated or open at the center of the segment. Optionally, an LED is embedded in the segment wall and the delay testing is performed on the segments in the assembled detector. These measurements can be performed periodically to partially compensate for instability or drift of the PMTs.
Optionally, alternatively or additionally, the PMTs and their associated circuitry are calibrated before assembly by feeding a light impulse of a standard intensity and timing into the PMT. The output of the circuitry is then measured and the gain and delay is noted and used to determine a correction factor for both energy measurement and timing. Optionally, the circuitry is adjusted to change the gain and time delay such that the outputs of all the PMTs have the same integrated signal output and timestamps.
Optionally, the PMTs can be removed from the rest of the segments so that they can be replaced, or adjusted when they go out of the calibration range.
If the segments are not separable (e.g., they are in a common liquid vessel) other methods can be used to determine energy and time delay corrections. In this case a collimated beam of high energy gammas (e.g., 1.4 MeV of K-40) is introduced perpendicular to the face of the detector. This beam has a substantial half length in the LS, before the first interaction and some of the interactions will be photoelectric interactions. The energy of these interactions is known and the difference in signals produced in the various segments (also as a function of position along the segments) is used to calibrate for energy. It can also be used to calibrate for position determination using signal strength, using the ratio of signals when the beam is at the center of the section as a standard correction for the ratios produced during detection of threats. This measurement can also define a relative difference in delay between the two end PMTs which can be used to determine the y position correction. As to absolute timing, this can be determined to a reasonable accuracy by the use of LEDs situated near each of the PMTs.
An additional source of reduction in gamma spectroscopic isotope ID quality is caused by energy that is lost when a residual gamma or electron escapes from the detector. While this phenomenon is well known, correcting for it is difficult, since it can not be determined on an individual basis if such escape occurred and also how much energy escaped. The result will be that the spectrum of a monoenergetic gamma source will have a lower energy pedestal as seen in
In an embodiment of this invention the incident Gamma particle signature of the Gamma particle with the segmented (or compartmentalized) detector (see
A background for this embodiment is given in the discussion of the Escape Quanta phenomenon associated with scintillation detectors (and especially with Organic Scintillators) spectroscopy in a book by G. Knoll “Radiation Detection and Measurement” (3rd edition) (see for example chapter 10 pages 307-322). The effects of “Escape Quanta” on energy determination and spectroscopy is also discussed in other parts of this (and cross referenced) PPA. Knoll shows that Escape Quanta can substantially degrade the determination of the energy of incident Gamma photons, since an unknown fraction of the incident energy is lost to escapes after some initial interactions inside the detector volume. In many applications, where multiple incident energies are present, the partial energy deposition of higher energies will frequently mask the complete energy deposition of lower ones, with no known way to tell those events apart. As shown in
The escaped energy quanta can be anywhere from a very small to a very large portion of the primary photon energy, rendering the energy measurement per event an upper bound at best, well short of useful energy assessment and identification.
It has been observed by the inventors of this PPA using a Monte Carlo simulations (that follow individual events inside the detector) that for the typical (40 KeV to 3 MeV) energy range incident gamma particles interacting with liquid scintillators (required to construct the system described in this application) there are typically about 30 Compton interactions in the detector before a final photoelectric absorption. It was also observed that most escapes, which are the ones that deteriorate gamma energy determination in large organic detectors (e.g. 40×200×200 cm), occur after a few (less than 10) Compton interactions. So if a gamma photon “survives” (or remains inside the detector volume) for the first few (e.g. ≧10) interactions, it is likely to remain inside for the entire interaction set until the final (e.g. photoelectric) interaction, in which case the entire incident energy will be deposited and measured. The Compton collisions (and its energy depositions) in the detector for an incident gamma particle occur at a fairly constant typical rate of several per nanosecond, thus the expected scintillation signals salvo will rise and stay roughly constant for the duration of the collision series, until the final interaction.
Thus, the present inventors have found, as confirmed by the above referenced simulations, that if the final detected scintillation is deep within the detector, the probability is high that all the energy of the incident particle is captured by the scintillator. The closer the final detected scintillation is to an outside surface of the detector, the higher the probability that there was an escape quanta of energy. Furthermore, the present inventors have discovered that if the time difference by the group of scintillations associated with the incoming radiation event is relatively long, then the probability is high that the all of the energy has been captured and that as the time difference decreases, there is a greater probability that there is an escape quanta. The number of scintillation events and the number of segments can also be used to indicate the probability of total energy capture, with the higher numbers representing a higher probability of complete energy capture.
To better understand this embodiment the reader is reminded that each identifiable scintillation generates a precise timestamp, deposited energy and its spatial location.
In one preferred embodiment which utilizes the incident gamma particle interaction with the (partitioned) detector bank to generate a full energy probability score, the following procedure can be used:
Let each sub-detector (cell) be identified by its unique coordinates as cell (I, j, k), and assume at least one of the sub-detectors (see
The scintillation measurements from all sub-detectors signals (which fall within specified spatial and temporal boundaries (e.g. +/−50 cm and +/−20 ns time/space volume) are collected.
This data set is used to determine a probability value Pfa that this event represents a gamma photon that was fully absorbed by the detector.
The number of scintillation events can be incorporated in the function or alternatively a threshold (for example 10 as indicated above) or can be used to veto events that produce less than the threshold number of scintillations.
It is noted that the population of the rejected particles may be used for applications which do not require accurate energy determination (e.g. spontaneous fission temporal based signature detection, coincidence based radioisotope identification).
The above embodiment with the possible addition of other available parameters that can be correlated to the probability of total absorption (e.g. maximal lateral spatial volume dimension of the group), is then used to weed out incident particles that are not likely to have deposited all its energy within the detector volume. This results in improved energy measurement fidelity of the remaining measurement.
The event temporal/spatial correlated scintillation volume can be selected by a combination of minimum dimension limits as mentioned above with a “quiescence” range—i.e. extend a given time/space dimension beyond the minimum limit if there is any touched cell near the limit.
While the probable direction of incidence of gammas associated with tracks 906 and 908 can only be estimated statistically, it is practically certain that the gamma ray that resulted in track 906 is incident from the front of the detector and that associated with track 908 is incident from the back of the detector. This is true for two reasons. First, the initial scintillation 907 of track 906 is nearer the front than the back face and the initial scintillation 909 of track 908 is nearer the back face. This provides a certain probability (depending on the mean free path of the gamma ray and the thickness of the detector) that the track resulting in 906 is caused by an incident ray passing through the front and the track resulting in 908 is caused by a ray passing through the back face. Thus, the sequence of scintillations or each track provides an indication of rear or front entry of the event.
In addition, the direction determined from the initial path of the track shows a high probability of incidence from the front for track 906 and from the back for 908.
In an embodiment of the invention, one or both of these factors (nearness and probable direction) are utilized to separate between gamma rays that enter from the front and those that enter from the back.
Track 910 corresponds to a gamma ray that has a much lower number of scintillations than normal. This is preferably classified as an event that for which not all the energy is captured. Such scintillations are preferably ignored.
The stored data is grouped by incident particles which are reconstructed and individually analyzed (1222). This process is described more fully with the aid of
The incident particle data is analyzed to determine one or more “signatures” (1242) characteristic of SNM, RDD and NORM and/or their isotopes. This is discussed more fully with respect to
Based on the individual signatures, a determination is as to whether a threat is present (1260). If a threat is identified with a high probability (e.g. >5σ), then an alarm is generated (1262). If multimodal analysis is available, then such analysis (1264), as described further below, is performed. If it is not available, then 1260, 1262 are replaced by 1280, 1282, 1284 and 1286, described immediately below. It should be noted that if multi-modal analysis is available, then it is usually performed before any alarm is sounded to verify the single modality determination and to reduce false alarms.
After multi-modal analysis, (and more preferably a plurality of multi-mode analyses) a threat assessment (1280) is performed. If the multi-modal threat probability is above a certain threshold, then an alarm is generated (1282), If it is below a second, lower threshold, then the vehicle/object being tested is cleared (1284). If it is between the two thresholds, then the vehicle/package is sent for further manual or machine testing (1286).
Returning to 1202, reference is made to
Returning to 1212, reference is made to
Returning to 1222,
First, the scintillations are grouped (1221) in accordance with their time stamps as scintillations that are generated by a single incident gamma or neutron. In practice, all scintillations that occur with a window of −10 nanosec and +20 nanosec of the “first” scintillation are considered as part of the same group, so long as they are geometrically close (e.g., closer than 1 meter apart). Since the time between incident particles is much larger than the time between scintillations, there is only a small chance of overlap of scintillations from different incident particles. In the event that there is such overlap, this in itself could be indicative of a cascaded event, spontaneous fission salvo or an RDD or of a very large unshielded source.
Once the scintillations have been grouped, the total energy (1232) transferred from the incoming event can be determined by summing the individual energy signals of the scintillations in the group.
Separately from the energy determination, the scintillations are sequenced (1223) based on their corrected time stamps. A time stamp for the incident radiation is determined as the first of the sequence of scintillations (1224) and its position of incidence is determined (1225) from the position along the segment as described above (for y) and by the segment in which it appears (x, z).
The sequence is optionally traced (1226) through the detector to determine its path. This path is optionally used to determine (1227) a gross direction of incidence. Depending on the energy, this gross direction can be used for rejecting (1228, 1229) events that are from terrestrial or sky sources and those that enter the detector from the sides other than the front face. For higher energy gamma, for which the scatter is relatively low, the gross direction becomes sharper and may be useful for imaging as well. Alternatively or additionally where collimation is available, a direction of incidence can be derived for one or both of gammas and neutrons, depending on the type and configuration of the collimation as described above.
Furthermore, using the principles described above, some of the events can be classified as having escape quanta (1230) and are either rejected for energy spectroscopic applications or alternatively their escape quanta energy is estimated, and this estimate is further used to calculate the incident particle total energy. The estimated total energy is given a probability factor which is used for spectroscopic and other particle energy dependent decisions (1231). The particle is then characterized (1233) by (1) its time of incidence; (2) its x, y incident coordinates; (3) its direction of incidence, if available; (4) whether it is a neutron or a gamma; and (5) its energy (if a gamma). This information is sent to 1240 for storage.
Returning to 1240,
First, information on reconstructed events that are stored is retrieved (1243). To the extent possible (depending on the detector capabilities) related events (for example gammas with a same energy or neutrons) are optionally imaged (1244).
Using the information that is stored in 1240 the following signature/analyses are possible: doublet/triplet coincidence (1245); gamma spectroscopy isotope ID (with or without imaging and on the entire detector or vehicle or only in the area of a possible threat) (1246); image based NORM ID to identify the NORM signature (1247); SNM-RDD “point” source ID (based on the understanding that threats are generally less than 0.5 meters in extent) (1248); neutron counting/imaging (1250); and spontaneous fission γ/N ID, based on the temporal coincidence of a gamma and/or neutron events (1251). When a modality produces an image, then this image can be superimposed on an optical image of the vehicle (1252). All of the generated analyses are sent to a single modality alarm (1260) which compares the level of the individual threats probability and determines if an alarm should be generated based on only a singe threat. These single modality analyses are then subject to multi-modal analysis 1264. It is well known in the art of statistics (and in particular in threat analysis) that probability of detection false alarm or overlooked threat rates can be significantly reduced when information from orthogonal sources (or semi-orthogonal sources) are available. Any of the techniques available in the art would appear to be suitable for the present multi-modal analysis. Some of the multimodal analyses include:
image guided gamma spectroscopic SNM-RDD ID;
closed circuit TV image of the object coupled with other signals or images;
combined Neutron counting and gamma spectroscopy ID;
doublet detection and Gamma Spectroscopy SNM-RDD-NORM ID;
doublet detection and imaging SNM-RDD-NORM ID; and
fused nuclear and gamma imaging.
Although the detectors are described in the context of threat detection of SNM-RDD devices and radioactive materials carried on vehicles, in some embodiments the large OS detectors are used to screen supply chain articles (e.g. containers, pallets, air cargo, mail bags, etc.)
While not described explicitly, corrections known in the art, such as background correction, can be applied in portals using detectors of the present invention.
In the description and claims of the present application, each of the verbs, “comprise” “include” and “have”, and conjugates thereof, are used to indicate that the object or objects of the verb are not necessarily a complete listing of members, components, elements or parts of the subject or subjects of the verb.
The present invention has been described using detailed descriptions of embodiments thereof that are provided by way of example and are not intended to limit the scope of the invention. The described embodiments comprise different features, not all of which are required in all embodiments of the invention. Some embodiments of the present invention utilize only some of the features or possible combinations of the features. Variations of embodiments of the present invention that are described and embodiments of the present invention comprising different combinations of features noted in the described embodiments will occur to persons of the art. The scope of the invention is limited only by the following claims.
|Cited Patent||Filing date||Publication date||Applicant||Title|
|US2950393||Nov 20, 1956||Aug 23, 1960||Bendix Corp||Gamma compensated neutron detector|
|US3076895||Apr 28, 1960||Feb 5, 1963||Gen Electric||Neutron detector|
|US3381131||May 4, 1965||Apr 30, 1968||Reuter Stokes Electronic Compo||Neutron detector for operation in high gamma fluxes|
|US3471414||Oct 15, 1968||Oct 7, 1969||Atomic Energy Commission||Castable neutron shield|
|US3670164||Aug 18, 1970||Jun 13, 1972||Atomic Energy Commission||Personnel plutonium monitor|
|US3688113||Jun 22, 1970||Aug 29, 1972||Univ Case Western Reserve||Tomographic radiation sensitive device|
|US3878373||Jun 30, 1971||Apr 15, 1975||Blum Alvin||Radiation detection device and a radiation detection method|
|US3899675||Mar 4, 1974||Aug 12, 1975||Cleon Corp||Whole body imaging|
|US3919557||May 15, 1974||Nov 11, 1975||Gen Electric||Whole body line scanner|
|US3935462||Mar 4, 1974||Jan 27, 1976||Cleon Corporation||Whole body imaging|
|US3956654||Feb 3, 1975||May 11, 1976||Westinghouse Electric Corporation||Long lived proportional counter neutron detector|
|US3960756||Aug 16, 1974||Jun 1, 1976||Bicron Corporation||High efficiency scintillation detectors|
|US3970852||Jul 8, 1974||Jul 20, 1976||Ohio Nuclear, Inc.||Process and apparatus for scanning sections of radiation|
|US3978337||Jan 29, 1975||Aug 31, 1976||Wisconsin Alumni Research Foundation||Three-dimensional time-of-flight gamma camera system|
|US3988585||Jun 5, 1975||Oct 26, 1976||Medical Data Systems Corporation||Three-dimensional rectilinear scanner|
|US4001591||Jul 11, 1975||Jan 4, 1977||Elscint Ltd.||Scintillation camera and head therefor having means for improving resolution over a limited field of view|
|US4021670||Sep 10, 1975||May 3, 1977||Noakes John E||Sealable high counting efficiency liquid scintillation vials|
|US4045676||Mar 13, 1975||Aug 30, 1977||Ortec Incorporated||Determining element concentrations in samples|
|US4060730||Sep 6, 1974||Nov 29, 1977||Elscint, Ltd.||Scintillation camera for establishing the coordinates of a radiation stimuli produced by a radiation field|
|US4095108||Sep 14, 1976||Jun 13, 1978||Elscint Ltd.||Signal processing equipment for radiation imaging apparatus|
|US4100413||Sep 14, 1976||Jul 11, 1978||Elscint Ltd.||Radiation imaging apparatus with improved accuracy|
|US4117330||Apr 21, 1977||Sep 26, 1978||Commissariat A L'energie Atomique||Gamma radiation detector|
|US4143271||Sep 14, 1976||Mar 6, 1979||Elscint Ltd.||Nuclear imaging device with improved linearity|
|US4149079||Jul 14, 1976||Apr 10, 1979||Elscint, Ltd.||Method of and means for scanning a body to enable a cross-section thereof to be reconstructed|
|US4179664||Jul 26, 1977||Dec 18, 1979||Ortec Incorporated||Constant fraction signal shaping apparatus|
|US4180736||Sep 25, 1978||Dec 25, 1979||The United States Of America As Represented By The United States Department Of Energy||Use of a large time-compensated scintillation detector in neutron time-of-flight measurements|
|US4200803||Apr 5, 1978||Apr 29, 1980||Kernforschungsanlage Julich Gesellschaft Mit Beschrankter Haftung||Multiple collimator apparatus with angularly adjustable collimator tubes|
|US4217497||Jun 16, 1978||Aug 12, 1980||The United States Of America As Represented By The Department Of Health, Education And Welfare||Portable instrument for measuring neutron energy spectra and neutron dose in a mixed n-γ field|
|US4243886||Jun 19, 1978||Jan 6, 1981||National Nuclear Corp.||Apparatus and method for the measurement of neutron moderating or absorbing properties of objects|
|US4262203||Feb 2, 1979||Apr 14, 1981||Overhoff Mario W||Alpha particle monitor|
|US4278885||May 2, 1979||Jul 14, 1981||Outokumpu Oy||Apparatus for measuring the concentrations of elements in a material by the capture gamma method|
|US4291227||Nov 2, 1979||Sep 22, 1981||The United States Of America As Represented By The United States Department Of Energy||Rapid scanning system for fuel drawers|
|US4322617||Feb 12, 1979||Mar 30, 1982||Fleit & Jacobson||Method and apparatus for calibrating a gamma counter|
|US4343994||Mar 21, 1980||Aug 10, 1982||Commissariat A L'energie Atomique||Particle detector and its production process|
|US4350607||Sep 11, 1978||Sep 21, 1982||Apfel Robert E||Detector and dosimeter for neutrons and other radiation|
|US4358682||Jul 7, 1980||Nov 9, 1982||Shell Oil Company||Neutron interface detector|
|US4369495||Jun 19, 1980||Jan 18, 1983||Elscint Ltd.||Method of and means for compensating for the dead time of a gamma camera|
|US4393307||Nov 10, 1980||Jul 12, 1983||Tokyo Shibaura Denki Kabushiki Kaisha||Neutron detectors|
|US4419578||Jun 15, 1981||Dec 6, 1983||United States Of America||Solid state neutron detector|
|US4424446||Jun 19, 1980||Apr 19, 1994||Elscint Ltd||Gamma camera correction system and method for using the same|
|US4426580||May 18, 1983||Jan 17, 1984||The United States Of America As Represented By The United States Department Of Energy||Detection device|
|US4429226||May 12, 1982||Jan 31, 1984||Elscint, Inc.||Method of and means for improving the resolution of a gamma camera|
|US4432059||Sep 3, 1980||Feb 14, 1984||Elscint Ltd.||Scanning gamma camera|
|US4434373||Sep 30, 1982||Feb 28, 1984||Richard Christ||Neutron shielding|
|US4447727||Jun 30, 1981||May 8, 1984||Irt Corporation||Large area neutron proportional counter and portal monitor detector|
|US4455616||Nov 18, 1981||Jun 19, 1984||Elscint, Ltd.||Fast gamma camera|
|US4476391||Mar 8, 1982||Oct 9, 1984||Mobil Oil Corporation||Method for improving accuracy in a neutron detector|
|US4481421||May 24, 1982||Nov 6, 1984||The United States Of America As Represented By The Secretary Of The Navy||Lithium-6 coated wire mesh neutron detector|
|US4493811||Jul 20, 1983||Jan 15, 1985||Tokyo Shibaura Denki Kabushiki Kaisha||Preamplifier for a wide range neutron flux monitoring system|
|US4498007||Jun 22, 1982||Feb 5, 1985||Rca Corporation||Method and apparatus for neutron radiation monitoring|
|US4509042||Mar 23, 1982||Apr 2, 1985||The United States Of America As Represented By The United States Department Of Energy||Portal radiation monitor|
|US4543485||Nov 19, 1982||Sep 24, 1985||Hitachi Chemical Company, Ltd.||Scintillator for radiation detection and process for producing the same|
|US4568510||Apr 12, 1983||Feb 4, 1986||Mobil Oil Corporation||Method and system for uranium exploration|
|US4573122||Nov 4, 1982||Feb 25, 1986||Elscint, Ltd.||Method of and means for compensating for the dead time of a gamma camera|
|US4580057||Apr 29, 1983||Apr 1, 1986||Mobil Oil Corporation||Neutron detector amplifier circuit|
|US4582670||Aug 24, 1982||Apr 15, 1986||Sentry Equipment Corporation||Counting system for radioactive fluids|
|US4588897||Apr 11, 1983||May 13, 1986||Elscint, Ltd.||Gamma camera correction system and method for using the same|
|US4588898||May 24, 1983||May 13, 1986||Kernforschungszentrum Karlsruhe Gmbh||Apparatus for measuring dose energy in stray radiation fields|
|US4598202||May 30, 1984||Jul 1, 1986||Walter Koechner||Nuclear and pressure sensitive line/perimeter detection system|
|US4613313||Dec 27, 1983||Sep 23, 1986||General Electric Company||Ionization detector|
|US4620100||Aug 26, 1983||Oct 28, 1986||General Electric Company||Automated monitoring of fissile and fertile materials in large waste containers|
|US4622466||Sep 12, 1984||Nov 11, 1986||Kabushiki Kaisha Toshiba||Pressure vessel of an X-ray detector|
|US4638158||Jan 18, 1984||Jan 20, 1987||Halliburton Company||Gamma ray measurement of earth formation properties using a position sensitive scintillation detector|
|US4731535||Feb 10, 1986||Mar 15, 1988||Firma Herfurth GmbH||Apparatus for checking persons for radioactive contamination|
|US4823016 *||Sep 15, 1987||Apr 18, 1989||Hamamatsu Photonics Kabushiki Kaisha||Scintillation detector for three-dimensionally measuring the gamma-ray absorption position and a positron CT apparatus utilizing the scintillation detector|
|US4841153 *||Jul 27, 1988||Jun 20, 1989||Cogent Limited||Coal analysis|
|US4864140 *||Aug 31, 1987||Sep 5, 1989||The University Of Michigan||Coincidence detection system for positron emission tomography|
|US4866277||Jun 2, 1988||Sep 12, 1989||Westinghouse Electric Corp.||Conveyor apparatus for detecting radioactive material in garments|
|US4870280||Dec 10, 1987||Sep 26, 1989||Hamamatsu Photonics Kabushiki||Radiation detector|
|US4937452||Nov 4, 1988||Jun 26, 1990||Ortec Incorporated||Charge trapping correction in photon detector systems|
|US5034610||Jun 1, 1990||Jul 23, 1991||Spacher Paul F||Mobile radiation monitor|
|US5041728||Dec 11, 1989||Aug 20, 1991||Rochester Gas And Electric Corpration||Portable personnel monitor which is collapsible for transporting and storage|
|US5078951||Aug 1, 1990||Jan 7, 1992||The United States Of America As Represented By The Secretary Of The Navy||High efficiency fast neutron threshold deflector|
|US5083026||Feb 12, 1990||Jan 21, 1992||Danev Elbaum||Method, apparatus and applications of the quantitation of multiple gamma-photon producing isotopes with increased sensitivity|
|US5155366 *||Aug 30, 1991||Oct 13, 1992||General Research Corporation||Method and apparatus for detecting and discriminating between particles and rays|
|US5204527||Mar 12, 1991||Apr 20, 1993||Halliburton Company||Neutron particle energy detector|
|US5315506||Dec 20, 1991||May 24, 1994||University Of Michigan||Correction for compton scattering by analysis of spatially dependent energy spectra employing regularization|
|US5317158||Oct 22, 1991||May 31, 1994||Martin Marietta Energy Systems, Inc.||Unitary scintillation detector and system|
|US5326974||Dec 19, 1990||Jul 5, 1994||Rautaruukki Oy, A Corp. Of Finland||Range-finding method and device|
|US5345084||Mar 29, 1993||Sep 6, 1994||The United States Of America As Represented By The United States Department Of Energy||Directional fast-neutron detector|
|US5440135||Sep 1, 1993||Aug 8, 1995||Shonka Research Associates, Inc.||Self-calibrating radiation detectors for measuring the areal extent of contamination|
|US5457720||Apr 15, 1994||Oct 10, 1995||General Electric Company||System for krypton-xenon concentration, separation and measurement for rapid detection of defective nuclear fuel bundles|
|US5517030||Oct 15, 1993||May 14, 1996||Nabais Conde; Carlos A.||Gas proportional scintillation counter for ionizing radiation with medium and large size radiation windows and/or detection volumes|
|US5532122||Oct 12, 1993||Jul 2, 1996||Biotraces, Inc.||Quantitation of gamma and x-ray emitting isotopes|
|US5638420||Jul 3, 1996||Jun 10, 1997||Advanced Research And Applications Corporation||Straddle inspection system|
|US5675151||Sep 15, 1995||Oct 7, 1997||Mitsubishi Denki Kabushiki Kaisha||Distribution type detector using scintillation fibers|
|US5692029||Jun 6, 1995||Nov 25, 1997||Technology International Incorporated||Detection of concealed explosives and contraband|
|US5721759||Nov 13, 1995||Feb 24, 1998||Ima Engineering Ltd. Oy||Method and equipment for determining the content of an element|
|US5734689||Jan 29, 1996||Mar 31, 1998||The United States Of America As Represented By The Secretary Of The Navy||Thermal neutron detector|
|US5738895||Apr 15, 1996||Apr 14, 1998||Good Humor-Breyers Ice Cream, Division Of Conopco, Inc.||Method and apparatus for producing a molded ice cream product|
|US5753919||May 9, 1996||May 19, 1998||Geolink (Uk) Limited||Gamma ray detection and measurement device|
|US5780856||Apr 18, 1996||Jul 14, 1998||Mitsubishi Denki Kabushiki Kaisha||Radiation detector and method of detecting radiation|
|US5821541||Jan 15, 1997||Oct 13, 1998||Tuemer; Tuemay O.||Method and apparatus for radiation detection|
|US5838759||Jun 5, 1997||Nov 17, 1998||Advanced Research And Applications Corporation||Single beam photoneutron probe and X-ray imaging system for contraband detection and identification|
|US5854489||Sep 13, 1996||Dec 29, 1998||Commissariat A L'energie Atomique||Method and device for correction of spectrometric measurements in the gamma photon detection field|
|US5880469||Feb 21, 1997||Mar 9, 1999||Miller; Thomas Gill||Method and apparatus for a directional neutron detector which discriminates neutrons from gamma rays|
|US6006162||May 29, 1997||Dec 21, 1999||Eg&G Ortec||Autocalibrating multichannel analyzer and method for use|
|US6076009||May 5, 1997||Jun 13, 2000||The University Of Michigan||Solid state beta-sensitive surgical probe|
|US6087663 *||Feb 5, 1998||Jul 11, 2000||Triumf||Segmented scintillation detector for encoding the coordinates of photon interactions|
|US6111257||Nov 21, 1997||Aug 29, 2000||Picker International, Inc.||Support assembly for scintillating crystal|
|US6120706||Feb 27, 1998||Sep 19, 2000||Bechtel Bwxt Idaho, Llc||Process for producing an aggregate suitable for inclusion into a radiation shielding product|
|US6134289||May 1, 1998||Oct 17, 2000||Battelle Memorial Institute||Thermal neutron detection system|
|US6149593||Dec 16, 1996||Nov 21, 2000||The Trustees Of The University Of Pennsylvania||Method and apparatus for detecting beta radiation|
|US6169285 *||Oct 23, 1998||Jan 2, 2001||Adac Laboratories||Radiation-based imaging system employing virtual light-responsive elements|
|US6175120||May 8, 1998||Jan 16, 2001||The Regents Of The University Of Michigan||High-resolution ionization detector and array of such detectors|
|US6184531||Apr 17, 1998||Feb 6, 2001||Battelle Memorial Institute||Apparatus for real-time airborne particulate radionuclide collection and analysis|
|US6194726||Sep 22, 1998||Feb 27, 2001||Digirad Corporation||Semiconductor radiation detector with downconversion element|
|US6201257||Jul 22, 1998||Mar 13, 2001||Advanced Scientific Concepts, Inc.||Semiconductor X-ray photocathodes devices|
|US6201530||May 29, 1998||Mar 13, 2001||Flashpoint Technology, Inc.||Method and system of optimizing a digital imaging processing chain|
|US6225634||Jun 29, 1998||May 1, 2001||Canberra Industries, Inc.||True coincidence summing correction for radiation detectors|
|US6228664||Feb 13, 1998||May 8, 2001||Canberra Industries, Inc.||Calibration method for radiation spectroscopy|
|US6255655||May 1, 2000||Jul 3, 2001||Smv America, Inc.||Gamma camera for PET and SPECT studies|
|US6255657||Sep 1, 1998||Jul 3, 2001||Bechtel Bwxt Idaho, Llc||Apparatuses and methods for detecting, identifying and quantitating radioactive nuclei and methods of distinguishing neutron stimulation of a radiation particle detector from gamma-ray stimulation of a detector|
|US6256373||Aug 16, 1999||Jul 3, 2001||Karl Bernstein||X-ray fluorescence instrument|
|US6271510||Aug 11, 1999||Aug 7, 2001||Izzie Boxen||Fiber optic gamma camera having scintillating fibers|
|US6285028||Jun 1, 1999||Sep 4, 2001||Kabushiki Kaisha Toshiba||Semiconductor radiation detector and nuclear medicine diagnostic apparatus|
|US6297506||Mar 23, 2000||Oct 2, 2001||John W. Young||System and method for reducing pile-up errors in multi-crystal gamma ray detector applications|
|US6298113||Feb 7, 2000||Oct 2, 2001||General Electric Company||Self aligning inter-scintillator reflector x-ray damage shield and method of manufacture|
|US6300635||Sep 10, 1997||Oct 9, 2001||Commissariat A L'energie Atomique||Low energy sensitive X-gamma dosimeter|
|US6341150||Jun 30, 2000||Jan 22, 2002||The Regents Of The University Of California||Fissile material detector|
|US6362477||Dec 10, 1998||Mar 26, 2002||Commonwealth Scientific And Industrial Research Organisation||Bulk material analyser for on-conveyor belt analysis|
|US6362485||Dec 2, 1997||Mar 26, 2002||British Nuclear Fuels Plc||Neutron radiation detector|
|US6369393||May 7, 1999||Apr 9, 2002||Canberra Industries, Inc.||Digital pulse de-randomization for radiation spectroscopy|
|US6380540||Jan 29, 1997||Apr 30, 2002||Ge Medical Systems Israel, Ltd.||Radiation imaging using simultaneous emission and transmission|
|US6380541||Oct 14, 1998||Apr 30, 2002||Commissariat A L'energie Atomique||Device for locating radiation sources|
|US6388260||Mar 6, 2000||May 14, 2002||Sandia Corporation||Solid state neutron detector and method for use|
|US6420710||Aug 14, 1997||Jul 16, 2002||Commissariat A L'energie Atomique||Device for spectrometric measurement in the field of gamma photon detection|
|US6423972||Nov 8, 1999||Jul 23, 2002||GSF - Forschungszentrum für Umwelt und Gesundheit GmbH||Method for determining neutron spectra and device for carrying out the method|
|US6448560||Jul 20, 1998||Sep 10, 2002||Tumay O. Tumer||Method and apparatus for gamma ray detection|
|US6452992||Jun 5, 1998||Sep 17, 2002||Commissariat A. L'energie Atomique||Method and device for measuring the relative proportions of plutonium and uranium in a body|
|US6456869||Mar 6, 2000||Sep 24, 2002||The Regents Of The University Of Michigan||Solid state beta-sensitive surgical probe|
|US6486486||Aug 17, 1999||Nov 26, 2002||Siemens Building Technologies Ag||Flame monitoring system|
|US6509563||Jul 27, 1999||Jan 21, 2003||Canberra Industries, Inc.||Method for reduction in the interference of cosmic ray-induced neutron events in passive neutron coincidence and multiplicity counting|
|US6519306||Aug 31, 2001||Feb 11, 2003||Hitachi, Ltd.||Neutron monitoring system|
|US6544442||Sep 22, 1999||Apr 8, 2003||Ut-Battelle, Llc||Method of loading organic materials with group III plus lanthanide and actinide elements|
|US6596998||Jul 31, 2000||Jul 22, 2003||Westinghouse Electric Company Llc||Method and system for identifying the source of a signal|
|US6603122||May 24, 2001||Aug 5, 2003||Ut-Battelle, Llc||Probe for contamination detection in recyclable materials|
|US6603124||Dec 21, 2001||Aug 5, 2003||Jean Maublant||Apparatus for detecting and locating a radioactive source emitting gamma rays and use of said apparatus|
|US6610977||Oct 1, 2001||Aug 26, 2003||Lockheed Martin Corporation||Security system for NBC-safe building|
|US6624415||Nov 15, 1999||Sep 23, 2003||Central Research Institute Of Electric Power Industry||Measuring method and device for radioactivity, radioactive concentration and radioactivity surface concentration|
|US6723996||Dec 7, 2000||Apr 20, 2004||Commissariat A L'energie Atomique||Variable collimation radiation detector|
|US6806475||Sep 27, 2000||Oct 19, 2004||British Nuclear Fuels, Plc||Methods and apparatus for investigating emissions|
|US6822235||Jul 15, 2002||Nov 23, 2004||Canberra Harwell Ltd.||Environmental radioactivity monitor|
|US6876711||Sep 24, 2001||Apr 5, 2005||Steven A. Wallace||Neutron detector utilizing sol-gel absorber and activation disk|
|US6906559||May 9, 2003||Jun 14, 2005||Tuemer Tuemay O.||Method and apparatus for gamma ray detection|
|US6944264||Nov 6, 2003||Sep 13, 2005||L-3 Communications Security And Detection Systems Corporation Delaware||Method and apparatus for transmitting information about a target object between a prescanner and a CT scanner|
|US6989541||May 30, 2003||Jan 24, 2006||General Dynamics Advanced Information Systems, Inc.||Coincident neutron detector for providing energy and directional information|
|US6992313||Sep 17, 2002||Jan 31, 2006||Adelphi Technology Inc.||X-ray and neutron imaging|
|US7026627||Dec 9, 2003||Apr 11, 2006||Delta Epsilon Instruments||Neutron/gamma ray survey instrument with directional gamma ray sensitivity|
|US7049603||Jul 26, 2004||May 23, 2006||Temple University Of The Commonwealth System Of Higher Education||Neutron source detection camera|
|US7151815||Apr 6, 2004||Dec 19, 2006||Westinghouse Electric Co Llc||Nonintrusive method for the detection of concealed special nuclear material|
|US7317195||Apr 8, 2005||Jan 8, 2008||Eikman Edward A||Quantitative transmission/emission detector system and methods of detecting concealed radiation sources|
|US7366282||Oct 15, 2005||Apr 29, 2008||Rapiscan Security Products, Inc.||Methods and systems for rapid detection of concealed objects using fluorescence|
|US7369640||Sep 1, 2006||May 6, 2008||Varian Medical Systems Technologies, Inc.||Radiation scanning of objects for contraband|
|US7521686||Aug 17, 2007||Apr 21, 2009||Trinity Engineering Associates, Inc.||Intrinsically directional fast neutron detector|
|US20010048730||Jun 5, 2001||Dec 6, 2001||Masumi Oshima||Method of highly sensitive analysis of nuclides by multiple gamma-ray detection|
|US20020036270||Jul 20, 1998||Mar 28, 2002||Tumay O. Tumer||Method and apparatus for gamma ray detection|
|US20020067789||Sep 24, 2001||Jun 6, 2002||Wallace Steven A.||Neutron detector utilizing sol-gel absorber and activation disk|
|US20020125429||Dec 7, 2000||Sep 12, 2002||Alain Lebrun||Variable Collimation radiation Detector|
|US20020175288||May 24, 2001||Nov 28, 2002||Rusi Taleyarkhan||Probe for contamination detection in recyclable materials|
|US20030006376||Jun 20, 2002||Jan 9, 2003||Tumer Tumay O.||Method and apparatus for radiation detection|
|US20030015655||Jul 15, 2002||Jan 23, 2003||Canberra Harwell Ltd.||Environmental radioactivity monitor|
|US20030081724||Sep 17, 2002||May 1, 2003||Piestrup Melvin A.||X-ray and neutron imaging|
|US20030111611||Dec 21, 2001||Jun 19, 2003||Jean Maublant||Apparatus for detecting and locating a radioactive source emitting gamma rays and use of said apparatus|
|US20030116713 *||Nov 15, 2002||Jun 26, 2003||Koninklijke Philips Electronics N.V.||Event localization and fall-off correction by distance-dependent weighting|
|US20030165211||May 29, 2002||Sep 4, 2003||Lee Grodzins||Detectors for x-rays and neutrons|
|US20030189510||Jan 2, 2002||Oct 9, 2003||Anderton Rupert N.||Imaging system and method|
|US20030197128||May 9, 2003||Oct 23, 2003||Tumer Tumay O.||Method and apparatus for gamma ray detection|
|US20030205677||Jun 4, 2003||Nov 6, 2003||British Nuclear Fuels Plc||Analysis of materials containing radioactive sources|
|US20030226971||Jun 11, 2002||Dec 11, 2003||Chandross Edwin Arthur||Nuclear radiation detector|
|US20040000645||Oct 11, 2001||Jan 1, 2004||David Ramsden||Gamma-ray spectrometry|
|US20040051044||Nov 13, 2001||Mar 18, 2004||Bjorn Bjurman||Device for determining the nuclide content of a radioactive fluid|
|US20040109532||Dec 4, 2002||Jun 10, 2004||John Ford||Radiation scanning units including a movable platform|
|US20040200966 *||Apr 18, 2002||Oct 14, 2004||David Ramsden||Gamma-ray detection apparatus and method for positron emission tomography|
|US20040251419||Aug 25, 2003||Dec 16, 2004||Nelson Robert Sigurd||Device and system for enhanced SPECT, PET, and Compton scatter imaging in nuclear medicine|
|US20050006589 *||Jun 27, 2003||Jan 13, 2005||Siemens Medical Solutions Usa, Inc.||Nuclear imaging system using scintillation bar detectors and method for event position calculation using the same|
|US20050011849||Jul 17, 2003||Jan 20, 2005||Nigel Chattey||Crane apparatus equipped with container security scanning system|
|US20050017181||Aug 19, 2004||Jan 27, 2005||The Regents Of The University Of Michigan||Method and system for high-speed, 3D imaging of optically-invisible radiation and detector and array of such detectors for use therein|
|US20050253073 *||Jul 17, 2002||Nov 17, 2005||Christian Joram||Gamma ray detector for positron emission tomography (pet) and single photon emisson computed tomography (spect)|
|US20050263711 *||May 10, 2005||Dec 1, 2005||Gfe Gesellschaft Fur Forschungsund Entwicklungsservice Mbh||High energy gamma probe with position sensing capability|
|US20050275545||Jul 23, 2004||Dec 15, 2005||Alioto John I||Inverse ratio of gamma-ray and neutron emissions in the detection of radiation shielding of containers|
|US20060011849||Jul 13, 2004||Jan 19, 2006||Institute Of Nuclear Energy Research, Atomic Energy Council||Gate monitoring system and method for instant gamma analysis|
|US20060017000||Jul 26, 2004||Jan 26, 2006||Martoff Charles J||Neutron source detection camera|
|US20060049357 *||Jan 28, 2005||Mar 9, 2006||Tumer Tumay O||Method and apparatus for radiation detection|
|US20060102845 *||Nov 15, 2004||May 18, 2006||General Electric Company||Method and apparatus for timing calibration in a PET scanner|
|US20060219932||May 13, 2004||Oct 5, 2006||Fellerman Andrew S||Tomography of solid materials|
|US20060284094||Feb 6, 2006||Dec 21, 2006||Dan Inbar||Detection of nuclear materials|
|US20060289775||Aug 8, 2006||Dec 28, 2006||Dan Inbar||Nuclear Threat Detection|
|US20070102646||Dec 14, 2004||May 10, 2007||Mark Goldberg||Method and system for detecting substances, such as special nuclear materials|
|US20070187608||Mar 23, 2007||Aug 16, 2007||Dan Inbar||Methods and Apparatus for Improved Gamma Spectra Generation|
|US20070205373||Aug 11, 2005||Sep 6, 2007||Navotek Medical Ltd.||Localization of a Radioactive Source Within a Body of a Subject|
|US20070210255||Feb 28, 2005||Sep 13, 2007||Paul Bjorkholm||Dual energy radiation scanning of objects|
|US20070278423||Apr 8, 2005||Dec 6, 2007||Eikman Edward A||Quantitative transmission/emission detector system and methods of detecting concealed radiation sources|
|US20080023631||Mar 14, 2007||Jan 31, 2008||Majors Harry W||Detector System for traffic lanes|
|US20080067390 *||May 13, 2005||Mar 20, 2008||David Ramsden||Gamma Ray Detectors|
|US20080135772||Dec 7, 2006||Jun 12, 2008||General Electric Company||Method and system for special nuclear material detection|
|US20080175351||Oct 12, 2007||Jul 24, 2008||The Regents Of The University Of California||Detecting special nuclear materials in suspect containers using high-energy gamma rays emitted by fission products|
|USRE36201||Apr 23, 1997||Apr 27, 1999||Miller; Thomas G.||High energy x-y neutron detector and radiographic/tomographic device|
|CN1405555A||Aug 14, 2001||Mar 26, 2003||清华大学||Aeronautical container/tray article examination system|
|DE10149888A1||Oct 10, 2001||Mar 27, 2003||Ise Ingenieurges Fuer Stillegu||Measurement of radioactive floor contamination in nuclear installations, by use of a program controlled vehicle that is driven automatically over the floor area and carries a radiation monitor for automatic radiation monitoring|
|EP0003811A3||Feb 16, 1979||Oct 31, 1979||Ditta FERRARI CLAUDIO di LUIGI FERRARI & C. S.p.A.||Method and plant for the heating and/or conditioning of rooms|
|EP0060574A1||Feb 8, 1982||Sep 22, 1982||UNC Nuclear Industries, Inc.||Portal type personnel radiation monitor|
|EP1026522A2||Dec 6, 1999||Aug 9, 2000||Valeo Schalter und Sensoren GmbH||Sytem and method to monitor an area to the side of a vehicle|
|RU2129289C1||Title not available|
|RU2150127C1||Title not available|
|RU2150693C1||Title not available|
|RU2158938C2||Title not available|
|RU2161299C2||Title not available|
|RU2191408C2||Title not available|
|RU2196980C1||Title not available|
|1||Offical Action Dated Oct. 27, 2009 From the US Patent and Trademark Office Re.: U.S. Appl. No. 11/348,040.|
|2||Official Action Dated Dec. 10, 2009 From the US Patent and Trademark Office Re.: U.S. Appl. No. 11/463,112.|
|3||Official Action Dated Jul. 24, 2008 From the US Patent and Trademark Office Re.: U.S. Appl. No. 11/463,112.|
|4||Official Action Dated Jun. 30, 2008 From the US Patent and Trademark Office Re.: U.S. Appl. No. 11/348,040.|
|5||Official Action Dated Mar. 3, 2009 From the US Patent and Trademark Office Re.: U.S. Appl. No. 11/348,040.|
|6||Official Action Dated May 1, 2009 From the US Patent and Trademark Office Re.: U.S. Appl. No. 11/463,112.|
|7||Official Action Dated May 25, 2010 From the US Patent and Trademark Office Re.: U.S. Appl. No. 11/348,040.|
|8||Official Action Dated May 27, 2010 From the US Patent and Trademark Office Re.: U.S. Appl. No. 11/463,112.|
|9||Official Action Dated Nov. 29, 2007 From the US Patent and Trademark Office Re.: U.S. Appl. No. 11/348,040.|
|10||Prussin et al. "Nuclear Car Wash Status Report, Aug. 2005", Lawrence Livermore National Laboratory, UCRL-TR-214636, p. 1-85, Aug. 16, 2005.|
|11||Response Dated Jan. 26, 2010 to Official Action of Dec. 10, 2009 From the US Patent and Trademark Office Re.: U.S. Appl. No. 11/463,112.|
|12||Response Dated Jan. 26, 2010 to Official Action of Oct. 27, 2009 From the US Patent and Trademark Office Re.: U.S. Appl. No. 11/348,040.|
|13||Slaughter et al. "Detection of Special Nuclear Material in Cargo Containers Using Neutron Interrogation", Lawrence Livermore National Laboratory, UCRL-ID-155315, p. 1-63, Aug. 2003.|
|14||Slaughter et al. "The‘Nuclear Car Wash’: A Scanner to Detect Illicit Special Nuclear Material in Cargo Containers", IEEE Sensors Journal, 5(4): 560-564, 2005.|
|15||Slaughter et al. "The'Nuclear Car Wash': A Scanner to Detect Illicit Special Nuclear Material in Cargo Containers", IEEE Sensors Journal, 5(4): 560-564, 2005.|
|Citing Patent||Filing date||Publication date||Applicant||Title|
|US8494808||May 17, 2011||Jul 23, 2013||The Johns Hopkins University||Method for optimizing parameters for detection systems|
|US9140804 *||Mar 30, 2012||Sep 22, 2015||General Electric Company||Methods and systems for determining timing recovery information in a positron emission tomography (PET) system|
|US9147503 *||Sep 21, 2011||Sep 29, 2015||Savannah River Nuclear Solutions, Llc||System and method for the identification of radiation in contaminated rooms|
|US20120043471 *||Sep 21, 2011||Feb 23, 2012||Harpring Lawrence J||Position an orientation determination system for a radiation detector|
|US20130256536 *||Mar 30, 2012||Oct 3, 2013||General Electric Company||Methods and systems for determining timing recovery information in a positron emission tomography (pet) system|
|Cooperative Classification||G01T1/167, G01V5/0091|
|European Classification||G01V5/00D8, G01T1/167|